Interaction of phospholipids with Ca2+ ions. On the role of the phospholipid head groups

Neutral phospholipids play an important role in Ca2+ binding to biomembranes, in particular if the membrane carries a net negative surface charge due to charged lipids or proteins. The concentration of Ca2+ ions in the plane of the phospholipid head groups can be enhanced by at least two orders of magnitude compared to bulk solution. Ca2+ binding furthermore changes the orientation of the phospholipid head groups which is accompanied by variations of the local membrane dipole potential of the order of 10(5) V/cm. Such high electric fields could entail conformational changes of membrane-bound proteins and the Ca2(+)-induced reorientation of the lipid dipoles could thus play a regulatory role in membrane function.     

Electric field-induced polarization of charged cell surface proteins does not determine the direction of galvanotaxis

Galvanotaxis, that is, migration induced by DC electric fields, is thought to play a significant role in development and wound healing, however, the mechanisms by which extrinsic electric fields orchestrate intrinsic motility responses are unknown. Using mammalian cell lines (3T3, HeLa, and CHO cells), we tested one prevailing hypothesis, namely, that electric fields polarize charged cell surface molecules, and that these polarized molecules drive directional motility. Negatively charged sialic acids, which contribute the bulk of cell surface charge, redistribute preferentially to the surface facing the direction of motility, as measured by labeling with fluorescent wheat germ agglutinin. We treated cells with neuraminidase to remove sialic acids; as expected, this decreased total cell surface charge. We also changed cell surface charge independent of sialic acid moieties, by conjugating cationic avidin to the surface of live cells. Neuraminidase inhibited the electric field-induced directional polarization of membrane ruffling and alpha4 integrin, while avidin treatment actually reversed the directional polarization of sialic acids. Neuraminidase treatment inhibited directionality but did not alter speed of motility. Surprisingly, avidin treatment did not significantly alter either directionality or speed of motility. Thus, our results demonstrate that electric field-induced polarization of charged species indeed occurs. However, polarization of the bulk of charged cell surface proteins is neither necessary nor sufficient to cause motility, thus contradicting the second part of our hypothesis. Because neuraminidase inhibited directional motility, we also conclude that sialic acids are required constituents of some cell surface molecule(s) through which electric fields mount a polarized transmembrane response.     

Evidences of plasma membrane-mediated ROS generation upon ELF exposure in neuroblastoma cells supported by a computational multiscale approach

BackgroundMolecular mechanisms of interaction between cells and extremely low frequency magnetic fields (ELF-MFs) still represent a matter of scientific debate. In this paper, to identify the possible primary source of oxidative stress induced by ELF-MF in SH-SY5Y human neuroblastoma cells, we estimated the induced electric field and current density at the cell level.MethodsWe followed a computational multiscale approach, estimating the local electric field and current density from the whole sample down to the single cell level. The procedure takes into account morphological modeling of SH-SY5Y cells, arranged in different topologies. Experimental validation has been carried out: neuroblastoma cells have been treated with Diphenyleneiodonium (DPI) -an inhibitor of the plasma membrane enzyme NADPH oxidase (Nox)- administered 24 h before exposure to 50 Hz (1 mT) MF.ResultsMacroscopic and microscopic dosimetric evaluations suggest that increased current densities are induced at the plasma membrane/extra-cellular medium interface; identifying the plasma membrane as the main site of the ELF-neuroblastoma cell interaction. The in vitro results provide an experimental proof that plasma membrane Nox exerts a key role in the redox imbalance elicited by ELF, as DPI treatment reverts the generation of reactive oxygen species induced by ELF exposure.General significanceMicroscopic current densities induced at the plasma membrane are likely to play an active physical role in eliciting ELF effects related to redox imbalance. Multiscale computational dosimetry, supported by an in vitro approach for validation, is proposed as the innovative and rigorous paradigm to unveil mechanisms underlying the complex ELF-MF interactions.     

Currents induced in anatomic models of the human for uniform and nonuniform power frequency magnetic fields

We have used the quasi-static impedance method to calculate the currents induced in the nominal 2 x 2 x 3 and 6 mm resolution anatomically based models of the human body for exposure to magnetic fields at 60 Hz. Uniform magnetic fields of various orientations and magnitudes 1 or 0.417 mT suggested in the ACGIH and ICNIRP safety guidelines are used to calculate induced electric fields or current densities for the various glands and organs of the body including the pineal gland. The maximum 1 cm(2) area-averaged induced current densities for the central nervous system tissues, such as the brain and the spinal cord, were within the reference level of 10 mA/m(2) as suggested in the ICNIRP guidelines for magnetic fields (0.417 mT at 60 Hz). Tissue conductivities were found to play an important role and higher assumed tissue conductivities gave higher induced current densities. We have also determined the induced current density distributions for nonuniform magnetic fields associated with two commonly used electrical appliances, namely a hair dryer and a hair clipper. Because of considerably higher magnetic fields for the latter device, higher induced electric fields and current densities were calculated.     

Plant actin controls membrane permeability

The biological effects of electric pulses with low rise time, high field strength, and durations in the nanosecond range (nsPEFs) have attracted considerable biotechnological and medical interest. However, the cellular mechanisms causing membrane permeabilization by nanosecond pulsed electric fields are still far from being understood. We investigated the role of actin filaments for membrane permeability in plant cells using cell lines where different degrees of actin bundling had been introduced by genetic engineering. We demonstrate that stabilization of actin increases the stability of the plasma membrane against electric permeabilization recorded by penetration of Trypan Blue into the cytoplasm. By use of a cell line expressing the actin bundling WLIM domain under control of an inducible promotor we can activate membrane stabilization by the glucocorticoid analog dexamethasone. By total internal reflection fluorescence microscopy we can visualize a subset of the cytoskeleton that is directly adjacent to the plasma membrane. We conclude that this submembrane cytoskeleton stabilizes the plasma membrane against permeabilization through electric pulses.     

Dielectric behavior of polyelectrolytes. IV. Electric polarizability of rigid biopolymers in electric fields

The equilibrium Kerr effect of a system of mobile charges constrained to the surface of biomacromolecules is calculated. Cylindrical and spherical geometries are considered. For the cylinder we determine the anisotropy of electric polarizability as a function of length, temperature, and number of charged species in the low-field regime, and the fraction of the maximum induced dipole in the field direction for higher electric fields. The results are compared to experimental data for DNA oligomers taken from the literature. With spherical geometry we calculate the fractional induced dipole moment as a function of electric field strength and from this deduce the orientation function. The field dependence of the orientation function is compared to experimental data in the literature for bovine disk membrane vesicles.     

About factors providing the fast protein-protein recognition in processes of complex formation

A package of programs for the examination of areas of subunit contacts (interface) in protein-protein (PP) complexes has been created and used for a detailed study of amino acid (AA) composition and interface structure in a large number of PP complexes from Brookhaven database (PBD). It appeared that in about 75% of the complexes, the AA composition of the subunit surface is not important. This suggests that, along with the surface AA composition, interactions between AA from the inner parts of protein globules may play a significant role in PP recognition. Such interactions between relatively distant AA residues can only be of electrostatic nature and contribute to the total electric field of the protein molecule. The configuration of the electric field itself appears to determine the PP recognition. The total electric field created by protein molecules can be calculated as a result of superimposition of the fields created by the protein multipole (i.e. by the totality of partial electric charges assigned to each atom of the molecule). We performed preliminary calculations for the distant electrostatic interaction of ribonuclease subunits in a vacuum. The results reveal that the effect of the electric fields of the protein multipole is strong enough to orient protein molecules prior to their Brown collision.     

Electric dichroism in the purple membrane of Halobacterium halobium.

Aqueous suspensions of fragments of the purple membrane of Halobacterium halobium are exposed to short electric field pulses. The relaxation kinetics of the induced dichroism are studied as a function of environmental factors such as temperature, medium viscosity, and treatment of the membranes with glutaraldehyde and dimethylsulfoxide. The data indicate that the alignment of the retinyl chromophore is due to orientation of the whole membrane fragments with their planes parallel to the electric field, as well as to an intramembrane orientation of bacteriorhodopsin molecules (or of a part of such molecules). Wavelength effects on the dichroic ratio show that weak, out of (membrane) plane components contribute to the chromophore spectrum on the red side (lambda greater than 560 nm) of the main (alpha) absorption band as well as the range of the beta band (lambda less than 480 nm). The former effect is attributed to exciton interactions, while the latter is assigned to the contribution of a transition to the lowest 1Ag+ state ("cis" band). It is also concluded that the transition moment along the short (kappa) axis, in the plane of the polyene molecule, has a substantial component perpendicular to the membrane plane.     

Electric Field-Induced Transmembrane Potential Depends on Cell Density and Organizatio

Electrochemotherapy is a novel technique to enhance the delivery of chemotherapeutic drugs into tumor cells. In this procedure, electric pulses are delivered to cancerous cells, which induce membrane permeabilization, to facilitate the passage of cytotoxic drugs through the cell membrane. This study examines how electric fields interact with and polarize a system of cells. Specifically, we consider how cell density and organization impact on induced cell transmembrane potential due to an external electric field. First, in an infinite volume of spherical cells, we examined how cell packing density impacts on induced transmembrane potential. With high cell density, we found that maximum induced transmembrane potential is suppressed and that the transmembrane potential distribution is altered. Second, we considered how orientation of cell sheets and strands, relative to the applied field, affects induced transmembrane potential. Cells that are parallel to the field direction suppress induced transmembrane potential, and those that lie perpendicular to the applied field potentiate its effect. Generally, we found that both cell density and cell organization are very important in determining the induced transmembrane potential resulting from an applied electric field.     

Synchronization of neuron population subject to steady DC electric field induced by magnetic stimulation

Electric fields, which are ubiquitous in the context of neurons, are induced either by external electromagnetic fields or by endogenous electric activities. Clinical evidences point out that magnetic stimulation can induce an electric field that modulates rhythmic activity of special brain tissue, which are associated with most brain functions, including normal and pathological physiological mechanisms. Recently, the studies about the relationship between clinical treatment for psychiatric disorders and magnetic stimulation have been investigated extensively. However, further development of these techniques is limited due to the lack of understanding of the underlying mechanisms supporting the interaction between the electric field induced by magnetic stimulus and brain tissue. In this paper, the effects of steady DC electric field induced by magnetic stimulation on the coherence of an interneuronal network are investigated. Different behaviors have been observed in the network with different topologies (i.e., random and small-world network, modular network). It is found that the coherence displays a peak or a plateau when the induced electric field varies between the parameter range we defined. The coherence of the neuronal systems depends extensively on the network structure and parameters. All these parameters play a key role in determining the range for the induced electric field to synchronize network activities. The presented results could have important implications for the scientific theoretical studies regarding the effects of magnetic stimulation on human brain.     

Orientation and linear dichroism of chloroplasts and sub-chloroplast fragments oriented in an electric field

Whole or broken spinach chloroplasts, bacterial chromatosphores and CPI chlorophyll · protein complexes in aqueous suspensions at room temperature can be oriented in externally applied electric fields. The orientation is observed by monitoring the electric field induced linear dichroism (LD). With whole chloroplasts a detectable LD signal is observed using voltages as low as 2–3 V (50 Hz alternating voltage) across an 0.3 cm electrode gap, and nearly complete orientation is observed at fields of 30 V · cm^?1. The wavelength dependence of the LD signals using either orienting electric fields ($\text{E}$) alone, or magnetic fields ($\text{B}$) alone, are similar but opposite in sign with $\text{E}$ and $\text{B}$ pointing in the same direction. The chloroplasts tend to orient in such a way that the membrane planes are parallel to $\text{E}$. The CPI complexes and bacterial chromatophores require much higher electric fields for orientation than whole chloroplasts (for CPI complexes E > 2000 V · cm^?1); rectangular, millisecond duration, voltage pulses are utilized for the observation of electric field induced LD spectra in these cases. Oriented CPI complexes exhibit LD maxima of the same sign at 685 and at 440 nm. The oriented chromatophores exhibit an LD spectrum of either positive or negative sign, depending on the wavelength. The mechanisms of the orientation are discussed.     

Attenuated total reflection IR spectroscopy as a tool to investigate the structure, orientation and tertiary structure changes in peptides and membrane proteins

During the last few years, attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) has become one of the most powerful methods to determine the structure of biological materials and in particular of components of biological membranes, like proteins that cannot be studied by x-ray crystallography and NMR. ATR-FTIR requires a little amount of material (1-100 microg) and spectra are recorded in a matter of minutes. The environment of the molecules can be modulated so that their conformation can be studied as a function of temperature, pressure, pH, as well as in the presence of specific ligands. For instance, replacement of amide hydrogen by deuterium is extremely sensitive to environmental changes and the kinetics of exchange can be used to detect tertiary conformational changes in the protein structure. Moreover, in addition to the conformational parameters that can be deduced from the shape of the infrared spectra, the orientation of various parts of the molecule can be estimated with polarized IR. This allows more precise analysis of the general architecture of the membrane molecules within the biological membranes. The present review focuses on ATR-IR as an experimental approach of special interest for the study of the structure, orientation, and tertiary structure changes in peptides and membrane proteins.     

Lipid-induced conformational transitions of beta-lactoglobulin

Bovine beta-lactoglobulin (betaLG) provides an excellent model protein system for beta-to-alpha conformational change, but its behavior varies when the change is induced by alcohols, surfactants, or lipid vesicles. Here the interaction and orientation of betaLG in association with various artificial lipid vesicles at neutral and acidic pH have been studied by use of several complementary spectroscopic techniques. Circular dichroism (CD) and Fourier transform infrared (FTIR) spectra demonstrated that betaLG acquires a non-native alpha-helical structure upon binding with anionic lipids, while zwitterionic lipids do not have a significant effect on its conformation. The degree of induced alpha-helix depends on the lipid concentration and is strongly affected by the charge of the protein and lipids as well as the ionic strength of the solution. Near-UV CD and Trp emission spectra revealed that the tertiary structure of lipid-bound betaLG is highly expanded but not completely disrupted. Fluorescence quenching together with a Trp emission blue shift showed that the Trp residues remain largely shielded from the solvent when interacting with DMPG, which would be consistent with at least some portions of betaLG having been inserted into the lipid membrane. The orientations of the alpha-helix and beta-sheet axes in membrane-bound betaLG were found to be parallel and perpendicular, respectively, to the membrane film normal, as determined by use of polarized attenuated total reflection (ATR) FTIR spectra. Our findings reveal that the lipid-induced beta-to-alpha transition in betaLG, accompanied by a substantial disruption in tertiary structure, is mainly driven by strong electrostatic interactions. Once the tightly packed betaLG is disrupted, hydrophobic residues become exposed and available for insertion into the lipid bilayer, where hydrophobic interaction with the lipids may play a role in stabilizing the helical components.     

Membrane structure of bombesin studied by infrared spectroscopy. Prediction of membrane interactions of gastrin-releasing peptide, neuromedin B, and neuromedin C

Bombesin, in contact with flat phospholipid bilayer membranes, was shown to adopt a membrane structure similar to that of substance P, dynorphin-(1-13)-tridecapeptide, and adrenocorticotropin-(1-24)-tetracosapeptide. The C-terminal message segment, comprising 8-10 amino acid residues, is inserted into a relatively hydrophobic membrane compartment as an alpha-helical domain oriented perpendicularly on the membrane surface. The N-terminal, hydrophilic tetrapeptide segment remains in the aqueous compartment as a random coil. This was shown with IR and IR attenuated total reflection spectroscopy. Equilibrium thermodynamic estimations confirmed the observed membrane structure with respect to helix length, strength of hydrophobic membrane association, and orientation (caused by favorably oriented molecular amphiphilic and helix electric dipole moments). The membrane structure may explain why Trp-8 and His-12 are essential for biologic activity. Neuromedin B is predicted to be able to adopt a membrane structure similar to that of bombesin. However, gastrin-releasing peptide and neuromedin C are predicted not to behave in the same manner. The molecular mechanism of receptor subtype selection by bombesin-like peptides may prove to be similar to that observed earlier for opioid peptides and the neurokinins.     

Reinterpretation of linear dichroism of chromatin supports a perpendicular linker orientation in the folded state

We present a reinterpretation of linear dichroism data for the salt induced condensation of chromatin. A conflict between electric and flow linear dichroism data for identical chromatin samples, studied at varying degrees of Mg2+ induced folding, can be solved if the orientation in electric fields is mainly determined through the polarization of counter ions along the linker parts, whereas the orientation in flow is governed by the hydrodynamical response of the entire chromatin fiber. The orientation of a chromatin fiber in an electric field would then depend on the linker tilt angle so that at an angle larger than 55 degrees the fiber would tend to orient perpendicular to the applied field. The different orientation distributions obtained with the two methods of alignment may in this way provide extra information about the structure and folding of chromatin.     

Changes in CNT-confined water structural properties induced by the variation in water molecule orientation

Using a (8, 8) carbon nanotube (CNT) as a model for nanochannel, we studied the effects of carbonyl (–CO) groups and external electric field on the properties of confined water molecules by molecular dynamics simulation. We analysed the density profiles, the distribution of orientation and the hydrogen bonds of water molecules in the axial and radial directions of the CNT. The results show that –CO groups are more powerful than electric fields on controlling water properties, and property changes induced by –CO groups are less affected by electric fields. Meanwhile, the particular behaviour of water molecules induced by the –CO groups is not limited near the –CO groups, but also expands to the whole CNT.     

Attraction, deformation and contact of membranes induced by low frequency electric fields

The force of attraction between erythrocyte ghosts induced by low frequency electric fields (60 Hz) was measured as a function of the intermembrane separation. It varied from 10(-14) N for separation of the order of the cell diameter to 10(-12) N for close approach and contact in 20 mM sodium phosphate buffers (conductivity 260 mS/m, pH 8.5). For large separations the interaction force followed a dependence on separation as predicted for dipole-dipole interactions. For small separation an empirical formula was obtained. The membranes deformed at close approach (less than 1 microns) before making contact. The contact area increased with time until reaching the final equilibrium state. The ghosts separated reversibly after switching off the electric field. The membrane tension induced by the ghost interaction at contact was estimated to be of the order of 0.1 mN/m. These first quantitative measurements of the force/separation dependence for intermembrane interactions induced by low frequency electric fields indicate that attractive forces, membrane deformation and contact area of cells depend strongly on intermembrane separation and field strength. The quantitative relationship between them are important for measuring membrane surface and mechanical properties, intermembrane forces and understanding mechanisms of membrane adhesion, instability and fusion in electric fields and in general.     

Reinterpretation of Linear Dichroism of Chromatin Supports a Perpendicular Linker Orientation in the Folded State

Abstract

We present a reinterpretation of linear dichroism data for the salt induced condensation of chromatin. A conflict between electric and flow linear dichroism data for identical chromatin samples, studied at varying degrees of Mg²⁺ induced folding, can be solved if the orientation in electric fields is mainly determined through the polarization of counter ions along the linker parts, whereas the orientation in flow is governed by the hydrodynamical response of the entire chromatin fiber. The orientation of a chromatin fiber in an electric field would then depend on the linker tilt angle so that at an angle larger than 55° the fiber would tend to orient perpendicular to the applied field. The different orientation distributions obtained with the two methods of alignment may in this way provide extra information about the structure and folding of chromatin.     

Kinetic Theory Model for Ion Movement through Biological Membranes: I. Field-Dependent Conductances in the Presence of Solution Symmetry

A model for ion movement through specialized sites in the plasma membrane is presented and analyzed using techniques from nonequilibrium kinetic theory. It is assumed that ions traversing these specialized regions interact with membrane molecules through central conservative forces. The membrane molecules are approximated as massive spherical scattering centers so that ionic fractional energy losses per collision are much less than one. Equations for steady-state membrane ionic currents and conductances as functions of externally applied electric field strength are derived and numerically analyzed, under the restriction of identical solutions on each size of the membrane and constant electric fields within the membrane. The analysis is carried through for a number of idealized ion-membrane molecule central force interactions. For any interaction leading to a velocity-dependent ion-membrane molecule collision frequency, the membrane chord conductance is a function of the externally applied electric field. Interactions leading to a collision frequency that is an increasing (decreasing) function of ionic velocity are characterized by chord conductances that are decreasing (increasing) functions of field strength. For ion-neutral molecule interactions, the conductance is such a rapidly decreasing function of field strength that the slope conductance becomes negative for all field strengths above a certain value.     

Mouse T lymphoma cells contain a transmembrane glycoprotein (GP85) that binds ankyrin

In this study we have used complementary biochemical and immunological techniques to establish that the lymphoma GP85 membrane glycoprotein is a transmembrane protein with a cytoplasmic domain that binds directly to ankyrin, a molecule known to link the membrane to the cytoskeleton. The evidence supporting our conclusion that the GP85 is a transmembrane glycoprotein is as follows: (a) GP85 can be surface-labeled with Na 125I and contains wheat germ agglutinin-binding sites, indicating that it has an extracellular domain; (b) GP85 can be phosphorylated by intracellular kinases, indicating that it has an intracellular domain; and (c) GP85 can be successfully incorporated into phospholipid vesicles, indicating the existence of a hydrophobic domain in the molecule. Further studies show that GP85 displays immunological cross-reactivity with the lymphocyte Pgp-1 (differentiation-specific) membrane glycoprotein, and with the erythrocyte anion transport membrane protein, band 3. Immunocytochemical studies indicate that an ankyrin-like protein accumulates underneath the lymphoma GP85 cap structure, suggesting an association of the ankyrin-like protein and GP85. This relationship has been further confirmed by the following results of binding and reconstitution experiments: (a) purified GP85 binds directly to an ankyrin-Sepharose column; (b) purified GP85 inserts into phospholipid vesicles in both the normal (right side out) and reversed (inside out) orientation (and with only the reversed configuration permits binding of ankyrin to GP85); and (c) cleavage of GP85 with trypsin yields a 40-kD peptide fragment that is part of the cytoplasmic domain and contains the ankyrin binding site(s). Based on these findings, we suggest that the lymphoma GP85 transmembrane glycoprotein contains a cytoplasmic domain that is directly involved in linking ankyrin to the cytoskeleton. This transmembrane linkage may play a pivotal role in receptor capping and cell activation in lymphocytes.